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3D chaotic mixing inside drops driven by transient electric field<br />
Xiumei Xu a and G. M. Homsy a<br />
We study the 3D chaotic trajectories inside a neutrally buoyant drop driven by<br />
periodically switching a uniform electric field through an angle . The extent of the<br />
chaotic mixing is related to two parameters: the angle and modulation period T. In a<br />
static electric field, the streamlines internal to the drop are axisymmetric Taylor<br />
circulations with two rings of center fixed points (CFP) at the top and bottom<br />
hemispheres corresponding to the vortex center. Periodically switching the field is<br />
equivalent to periodically changing the axis of symmetry, and thus the position of<br />
these CFPs. There are always common CFPs during the field rotation, and there are<br />
either 4 or 8 depending on the range of . When equals /2, although the<br />
trajectories are three dimensional, Poincare maps show that for all modulating periods,<br />
the 3D trajectories are confined to certain KAM surfaces, determined only by initial<br />
positions, which limit the mixing. For other than /2, chaotic mixing is generated<br />
inside the drop, but there are ordered regions near the common CFPs, with more<br />
regions for the larger number of common CFPs (Figure 1). Inside the ordered regions,<br />
trajectories move around the common CFPs in complicated way, and the Poincare<br />
maps can exhibit highly ordered fractal structures. The mixing also depends on the<br />
modulating period, and our numerical results show that by modifying T it is possible<br />
to break the ordered islands and achieve global chaotic mixing. These results suggest<br />
there are optimum operating conditions that maximize mixing.<br />
a University of California-Santa Barbara, Santa Barbara, 93106, USA<br />
z<br />
(a) (b)<br />
z<br />
y y<br />
Figure 1: Typical Poincare maps, T=6, (a) =0.45 , the case of 8 common center<br />
fixed points; (b) =0.25 , the case of 4 common center fixed points.<br />
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